This is an R Markdown Notebook. When you execute code within the notebook, the results appear beneath the code.

library(ggplot2)
library(plyr)
library(readr)
library(dplyr)
library(glmnet)
library(tibble) 
library(caret)
library(RColorBrewer)
library(pheatmap)
library(dslabs)
library(forcats)
library(reshape2)
library(tidyr)

day = read.csv("/Users/Murphy1/Desktop/DATA2020/Project2020/data/hour.csv", header = TRUE)
head(day)
day2 <- head(day, 8646)

plot <- ggplot(data = day2, aes(x = day2$dteday, y = day2$cnt)) +
  geom_point(color = "brown") + 
  xlab('date') +ylab('count')
plot +  theme(axis.ticks.x=element_blank(),
              axis.text.x=element_blank()) + 
  ggtitle('check seasonaility')

NA
#select variables season, workingday, weathersit, temp, atemp, hum, windspeed
day1 <- dplyr::select(day, -c(instant, dteday))
head(day1)
plot <- ggplot(data = day1, aes(x = season, y = cnt, fill = factor(day1$season)))
plot + geom_boxplot() + scale_fill_brewer(palette = "YlOrBr") + 
  ylab('count') + 
  theme(panel.grid.major = element_blank(), panel.grid.minor = element_blank(),
panel.background = element_blank(), axis.line = element_line(colour = "black")) +
  ggtitle('count vs. seasonality')

plot <- ggplot(day1, aes(x = day1$cnt)) + 
  geom_histogram(aes(y = ..density..), bins = 30, fill = "wheat") +
  geom_density(color = "brown") + xlab('count')
plot + theme(panel.grid.major = element_blank(), panel.grid.minor = element_blank(),
panel.background = element_blank(), axis.line = element_line(colour = "black")) +
  ggtitle('distribution of count')


day1 <- lapply(day1, function(x) as.numeric(x))
day1 <- data.frame(day1)

y <- day1$cnt
X <- dplyr::select(day1, -c(cnt))

corr <- round(cor(X),2)

get_upper_tri<-function(corr){
    corr[lower.tri(corr, diag=TRUE)] <- NA
    return(corr)
}
upper <- get_upper_tri(corr)
melted_upper <- melt(upper, na.rm=TRUE)

ggplot(data = melted_upper, aes(Var2, Var1, fill = value))+
 geom_tile(color = "white")+
 scale_fill_gradient2(low = "wheat", high = "brown", mid = "white", 
   midpoint = 0, limit = c(-1,1), space = "Lab") +
  theme(
  axis.text.x = element_text(angle = 45, vjust = 1, 
    size = 4, hjust = 1),
  axis.title.x = element_blank(),
  axis.title.y = element_blank(),
  panel.grid.major = element_blank(),
  panel.border = element_blank(),
  panel.background = element_blank(),
  axis.ticks = element_blank())+
  geom_text(aes(Var2, Var1, label = value), color = "gray", size = 2.8) +
  coord_fixed() +
  labs(fill='correlation')  + ggtitle('correlation heatmap')

#drop atemp
day1 <- dplyr::select(day1, -c(atemp))
day1
# Check Line

fit.all = lm(cnt ~ season + yr + mnth + hr + holiday + workingday + weathersit + temp + hum + windspeed, data = day1)

intercept_only <- lm(cnt ~ 1, data=day1)

forward <- step(intercept_only, direction='forward', 
                scope=formula(fit.all))
Start:  AIC=180764.7
cnt ~ 1

             Df Sum of Sq       RSS    AIC
+ temp        1  93677759 478083832 177657
+ hr          1  88790198 482971393 177834
+ hum         1  59618351 512143240 178853
+ yr          1  35876722 535884870 179641
+ season      1  18127040 553634551 180207
+ weathersit  1  11598301 560163290 180411
+ mnth        1   8321115 563440476 180512
+ windspeed   1   4970060 566791531 180615
+ holiday     1    546889 571214702 180750
+ workingday  1    524387 571237204 180751
<none>                    571761591 180765

Step:  AIC=177657
cnt ~ temp

             Df Sum of Sq       RSS    AIC
+ hr          1  66728221 411355610 175046
+ hum         1  49874585 428209247 175744
+ yr          1  31342263 446741569 176481
+ windspeed   1   6021342 472062489 177439
+ weathersit  1   5880680 472203151 177444
+ season      1   1696802 476387030 177597
+ mnth        1    906463 477177369 177626
+ holiday     1    225697 477858135 177651
<none>                    478083832 177657
+ workingday  1     35467 478048365 177658

Step:  AIC=175046.4
cnt ~ temp + hr

             Df Sum of Sq       RSS    AIC
+ yr          1  32229070 379126540 173631
+ hum         1  25434149 385921461 173939
+ weathersit  1   5638993 405716617 174809
+ season      1   2995571 408360039 174921
+ windspeed   1   1712372 409643238 174976
+ mnth        1   1525503 409830107 174984
+ holiday     1    260174 411095436 175037
+ workingday  1     54016 411301595 175046
<none>                    411355610 175046

Step:  AIC=173630.5
cnt ~ temp + hr + yr

             Df Sum of Sq       RSS    AIC
+ hum         1  20865128 358261412 172649
+ weathersit  1   5240157 373886383 173391
+ season      1   3515639 375610901 173471
+ mnth        1   1811568 377314972 173549
+ windspeed   1   1810495 377316045 173549
+ holiday     1    307712 378818828 173618
+ workingday  1     66617 379059923 173629
<none>                    379126540 173631

Step:  AIC=172648.7
cnt ~ temp + hr + yr + hum

             Df Sum of Sq       RSS    AIC
+ season      1   7325038 350936374 172292
+ mnth        1   4840141 353421271 172414
+ holiday     1    367007 357894405 172633
+ weathersit  1    133898 358127514 172644
+ workingday  1    117604 358143808 172645
<none>                    358261412 172649
+ windspeed   1     15517 358245895 172650

Step:  AIC=172291.7
cnt ~ temp + hr + yr + hum + season

             Df Sum of Sq       RSS    AIC
+ holiday     1    371167 350565206 172275
+ windspeed   1    165365 350771008 172286
+ workingday  1    131868 350804506 172287
<none>                    350936374 172292
+ weathersit  1     37972 350898402 172292
+ mnth        1       799 350935575 172294

Step:  AIC=172275.3
cnt ~ temp + hr + yr + hum + season + holiday

             Df Sum of Sq       RSS    AIC
+ windspeed   1    165343 350399863 172269
+ workingday  1     47102 350518104 172275
+ weathersit  1     42022 350523184 172275
<none>                    350565206 172275
+ mnth        1         0 350565206 172277

Step:  AIC=172269.1
cnt ~ temp + hr + yr + hum + season + holiday + windspeed

             Df Sum of Sq       RSS    AIC
+ weathersit  1     73738 350326125 172267
+ workingday  1     48197 350351667 172269
<none>                    350399863 172269
+ mnth        1         1 350399863 172271

Step:  AIC=172267.5
cnt ~ temp + hr + yr + hum + season + holiday + windspeed + weathersit

             Df Sum of Sq       RSS    AIC
+ workingday  1     53900 350272225 172267
<none>                    350326125 172267
+ mnth        1         1 350326124 172269

Step:  AIC=172266.8
cnt ~ temp + hr + yr + hum + season + holiday + windspeed + weathersit + 
    workingday

       Df Sum of Sq       RSS    AIC
<none>              350272225 172267
+ mnth  1      1.92 350272223 172269
summary(forward)

Call:
lm(formula = cnt ~ temp + hr + yr + hum + season + holiday + 
    windspeed + weathersit + workingday, data = day1)

Residuals:
    Min      1Q  Median      3Q     Max 
-366.86  -93.52  -27.97   60.40  644.46 

Coefficients:
             Estimate Std. Error t value Pr(>|t|)    
(Intercept)   -9.4775     6.5712  -1.442 0.149246    
temp         282.8600     6.0073  47.086  < 2e-16 ***
hr             7.6962     0.1649  46.680  < 2e-16 ***
yr            80.9848     2.1668  37.376  < 2e-16 ***
hum         -197.1206     6.8663 -28.708  < 2e-16 ***
season        20.0853     1.0486  19.154  < 2e-16 ***
holiday      -25.1349     6.6610  -3.773 0.000162 ***
windspeed     29.5888     9.4015   3.147 0.001651 ** 
weathersit    -3.7797     1.9044  -1.985 0.047187 *  
workingday     3.9204     2.3980   1.635 0.102096    
---
Signif. codes:  0 ‘***’ 0.001 ‘**’ 0.01 ‘*’ 0.05 ‘.’ 0.1 ‘ ’ 1

Residual standard error: 142 on 17369 degrees of freedom
Multiple R-squared:  0.3874,    Adjusted R-squared:  0.3871 
F-statistic:  1220 on 9 and 17369 DF,  p-value: < 2.2e-16
#forward
backward <- step(fit.all, direction='backward')
Start:  AIC=172268.8
cnt ~ season + yr + mnth + hr + holiday + workingday + weathersit + 
    temp + hum + windspeed

             Df Sum of Sq       RSS    AIC
- mnth        1         2 350272225 172267
<none>                    350272223 172269
- workingday  1     53901 350326124 172269
- weathersit  1     79432 350351655 172271
- windspeed   1    199754 350471977 172277
- holiday     1    286716 350558939 172281
- season      1   2453586 352725809 172388
- hum         1  16562243 366834466 173070
- yr          1  28170183 378442406 173611
- hr          1  43896453 394168676 174319
- temp        1  44245313 394517536 174334

Step:  AIC=172266.8
cnt ~ season + yr + hr + holiday + workingday + weathersit + 
    temp + hum + windspeed

             Df Sum of Sq       RSS    AIC
<none>                    350272225 172267
- workingday  1     53900 350326125 172267
- weathersit  1     79442 350351667 172269
- windspeed   1    199752 350471977 172275
- holiday     1    287145 350559370 172279
- season      1   7398820 357671045 172628
- hum         1  16620569 366892794 173070
- yr          1  28171966 378444191 173609
- hr          1  43943958 394216183 174319
- temp        1  44711469 394983694 174353
summary(backward)

Call:
lm(formula = cnt ~ season + yr + hr + holiday + workingday + 
    weathersit + temp + hum + windspeed, data = day1)

Residuals:
    Min      1Q  Median      3Q     Max 
-366.86  -93.52  -27.97   60.40  644.46 

Coefficients:
             Estimate Std. Error t value Pr(>|t|)    
(Intercept)   -9.4775     6.5712  -1.442 0.149246    
season        20.0853     1.0486  19.154  < 2e-16 ***
yr            80.9848     2.1668  37.376  < 2e-16 ***
hr             7.6962     0.1649  46.680  < 2e-16 ***
holiday      -25.1349     6.6610  -3.773 0.000162 ***
workingday     3.9204     2.3980   1.635 0.102096    
weathersit    -3.7797     1.9044  -1.985 0.047187 *  
temp         282.8600     6.0073  47.086  < 2e-16 ***
hum         -197.1206     6.8663 -28.708  < 2e-16 ***
windspeed     29.5888     9.4015   3.147 0.001651 ** 
---
Signif. codes:  0 ‘***’ 0.001 ‘**’ 0.01 ‘*’ 0.05 ‘.’ 0.1 ‘ ’ 1

Residual standard error: 142 on 17369 degrees of freedom
Multiple R-squared:  0.3874,    Adjusted R-squared:  0.3871 
F-statistic:  1220 on 9 and 17369 DF,  p-value: < 2.2e-16

day2 <- day1 %>% dplyr::select(-c(casual, registered))
#day2
day2$cnt <- log(day2$cnt)
#day2
x <- model.matrix(day2$cnt~., day2)[,-1]
y <- day2 %>% dplyr::select(cnt) %>% unlist() %>% as.numeric()

#y
grid <- 10^seq(2, -3, by=-.1)

train <- day2 %>% sample_frac(0.8)
test <- day2 %>% setdiff(train)

x_train <- model.matrix(train$cnt~., train)[,-1]
x_test <- model.matrix(test$cnt~., test)[,-1]
cnt <- day2$cnt
#cnt
y_train <- train %>% dplyr::select(cnt) %>% unlist() %>% as.numeric()
y_test <- test %>% dplyr::select(cnt) %>% unlist() %>% as.numeric()
set.seed(1)

#on the full model
out <- glmnet(x, y, alpha = 1, lambda = grid) 

#cv to choose best lambda
cv.out <- cv.glmnet(x_train, y_train, alpha = 1) 
bestlam <- cv.out$lambda.min 
cat('Best lambda obtained is: ', bestlam)
Best lambda obtained is:  0.002401653
#lasso with best lambda
lasso <- glmnet(x, y, alpha = 1, lambda = bestlam)
predictions <- predict(lasso, type = "coefficients", s = bestlam)
#coef(lasso, s=bestlam)

#remove intercept
lasso.mod <- glmnet(x,y, alpha =1)
beta <- coef(lasso.mod)
beta <- as.matrix(beta)
dim(beta)
[1] 12 64
lambda <- lasso.mod$lambda
length(lambda)
[1] 64
lam <- rep(lambda, 11)
length(lam)
[1] 704
beta_t <- t(beta)
beta_vec <- as.vector(beta_t)[-c(1:64)]
length(beta_vec)
[1] 704
v <- rownames(beta)[-1]
length(v)
[1] 11
names <- rep(v, each=64)
length(beta_vec)
[1] 704
length(names)
[1] 704
df <- data.frame(lam, names, beta_vec)
plot <- ggplot(df, aes(x = lam, y = beta_vec, color = names)) +
  geom_line() +
  labs(x = "log(lambda)", y = "Coefficient") +
  theme_bw() +
  scale_x_continuous(trans='log10')

plot + ggtitle('Lasso coefficients vs. lambda')

#x_test
lasso_pred <- predict(lasso, newx = x_test, s = bestlam)
#y_test

#lasso_pred
mae <- mean(abs(y_test - lasso_pred))
mse <- mean((y_test - lasso_pred)^2)
r_squared <- 1 - (sum((y_test- lasso_pred)^2) / sum((y_test - mean(y_test))^2))
mae
[1] 0.8257472
mse
[1] 1.101616
r_squared
[1] 0.4764416
day1$cnt <- log(day1$cnt)
mod_forward <- lm(formula = cnt ~ temp + hr + yr + hum + season + holiday + 
    windspeed + weathersit + workingday, data = day1)
plot(mod_forward, which = c(1,2,3,4))

mod_backward <- lm(formula = cnt ~ season + yr + hr + holiday + workingday + 
    weathersit + temp + hum + windspeed, data = day1)
plot(mod_backward, which = c(1,2,3,4))

# Check the variance 
library(car)
ncvTest(fit.all)
Non-constant Variance Score Test 
Variance formula: ~ fitted.values 
Chisquare = 2063.008, Df = 1, p = < 2.22e-16


set.seed(42)
train_index <- createDataPartition(day1$cnt, p = 0.8, list = FALSE)
train_set <- day1[train_index,]
test_set <- day1[-train_index,]

# Train the multiple linear regression model
model <- lm(formula = cnt ~ season + yr + hr + holiday + workingday + 
    weathersit + temp + hum + windspeed, data = train_set)

# Make predictions on the test set
predictions <- predict(model, newdata = test_set)

# Evaluate the model
mae <- mean(abs(test_set$cnt - predictions))
mse <- mean((test_set$cnt - predictions)^2)
r_squared <- 1 - (sum((test_set$cnt - predictions)^2) / sum((test_set$cnt - mean(test_set$cnt))^2))

cat('Mean Absolute Error:', mae, '\n')
Mean Absolute Error: 0.8430607 
cat('Mean Squared Error:', mse, '\n')
Mean Squared Error: 1.156954 
cat('R-squared:', r_squared, '\n')
R-squared: 0.4713828 
rmse <- function(actual, predicted) {
  return(sqrt(mean((actual - predicted)^2)))
}
rmse_value <- rmse(test_set$cnt, predictions)
cat('Root Mean Squared Error:', rmse_value, '\n')
Root Mean Squared Error: 1.075618 
plot(cnt ~ temp + hr + yr + hum + season + holiday + 
    windspeed + weathersit + workingday, data = day1)

day2 <- day1[ , -which(names(day1) == "cnt")]
pca <- prcomp(day2,scale=TRUE)
variance <- summary(pca)$importance[2,]
df <- data.frame(Component = 1:length(variance), Variance = variance)
df_top_10 <- df[1:10,]
df_top_10 <- df_top_10[order(-df_top_10$Variance),]
df_top_10

pc <- pca$rotation[, 1: 10]
z <- melt(pc)
colnames(z) <- c("Variable", "PC", "value")
plot <- ggplot(z, aes(x = PC, y = Variable, fill= value)) +
 geom_tile(color = 'white')+
 scale_fill_gradient2(low = 'brown', high = 'wheat', mid = 'ivory',
   midpoint = 0, limit = c(-1,1), space = 'Lab')
plot


pca_data <- as.data.frame(predict(pca))
df2 <- pca_data[, 1:2]
df1 <- subset(day1, select = cnt)
combined_df <- cbind(df1, df2)

train_index <- createDataPartition(combined_df$cnt, p = 0.8, list = FALSE)
train_set <- combined_df[train_index,]
test_set <- combined_df[-train_index,]
# Train the multiple linear regression model
model2 <- lm(cnt ~ ., data = train_set)
summary(model2)

Call:
lm(formula = cnt ~ ., data = train_set)

Residuals:
    Min      1Q  Median      3Q     Max 
-3.9418 -0.4606  0.1181  0.6162  2.7952 

Coefficients:
            Estimate Std. Error t value Pr(>|t|)    
(Intercept) 4.537284   0.007966  569.55   <2e-16 ***
PC1         0.720840   0.005032  143.24   <2e-16 ***
PC2         0.113545   0.005553   20.45   <2e-16 ***
---
Signif. codes:  0 ‘***’ 0.001 ‘**’ 0.01 ‘*’ 0.05 ‘.’ 0.1 ‘ ’ 1

Residual standard error: 0.9394 on 13901 degrees of freedom
Multiple R-squared:  0.601, Adjusted R-squared:  0.601 
F-statistic: 1.047e+04 on 2 and 13901 DF,  p-value: < 2.2e-16
# Make predictions on the test set
predictions <- predict(model2, newdata = test_set)
# Evaluate the model
mae <- mean(abs(test_set$cnt - predictions))
mse <- mean((test_set$cnt - predictions)^2)
r_squared <- 1 - (sum((test_set$cnt - predictions)^2) / sum((test_set$cnt - mean(test_set$cnt))^2))
summary(predictions)
   Min. 1st Qu.  Median    Mean 3rd Qu.    Max. 
  1.916   3.689   4.405   4.555   5.292   8.573 
r_squared
[1] 0.590504
mae
[1] 0.7150052
mse
[1] 0.8998416
ggplot(df_top_10, aes(x = factor(Component), y = Variance)) +
  geom_bar(stat = "identity", fill = "wheat") +
  scale_x_discrete(labels = 1:10) +
  theme(panel.background = element_rect(fill = "white")) +
  labs(x = "Principal Component", y = "Proportion of Variance Explained",
       title = "Proportion of Variance Explained by Top 10 Principal Components")+
  theme(legend.position = "none")

---
title: "DATA 2020"
output: html_notebook
---

This is an [R Markdown](http://rmarkdown.rstudio.com) Notebook. When you execute code within the notebook, the results appear beneath the code. 


```{r}
library(ggplot2)
library(plyr)
library(readr)
library(dplyr)
library(glmnet)
library(tibble) 
library(caret)
library(RColorBrewer)
library(pheatmap)
library(dslabs)
library(forcats)
library(reshape2)
library(tidyr)

day = read.csv("/Users/Murphy1/Desktop/DATA2020/Project2020/data/hour.csv", header = TRUE)
head(day)
day2 <- head(day, 8646)

plot <- ggplot(data = day2, aes(x = day2$dteday, y = day2$cnt)) +
  geom_point(color = "brown") + 
  xlab('date') +ylab('count')
plot +  theme(axis.ticks.x=element_blank(),
              axis.text.x=element_blank()) + 
  ggtitle('check seasonaility')
  
```
```{r, include=TRUE}
#select variables season, workingday, weathersit, temp, atemp, hum, windspeed
day1 <- dplyr::select(day, -c(instant, dteday))
head(day1)
plot <- ggplot(data = day1, aes(x = season, y = cnt, fill = factor(day1$season)))
plot + geom_boxplot() + scale_fill_brewer(palette = "YlOrBr") + 
  ylab('count') + 
  theme(panel.grid.major = element_blank(), panel.grid.minor = element_blank(),
panel.background = element_blank(), axis.line = element_line(colour = "black")) +
  ggtitle('count vs. seasonality')
```
```{r}
plot <- ggplot(day1, aes(x = day1$cnt)) + 
  geom_histogram(aes(y = ..density..), bins = 30, fill = "wheat") +
  geom_density(color = "brown") + xlab('count')
plot + theme(panel.grid.major = element_blank(), panel.grid.minor = element_blank(),
panel.background = element_blank(), axis.line = element_line(colour = "black")) +
  ggtitle('distribution of count')
```

```{r, include=TRUE}

day1 <- lapply(day1, function(x) as.numeric(x))
day1 <- data.frame(day1)

y <- day1$cnt
X <- dplyr::select(day1, -c(cnt))

corr <- round(cor(X),2)

get_upper_tri<-function(corr){
    corr[lower.tri(corr, diag=TRUE)] <- NA
    return(corr)
}
upper <- get_upper_tri(corr)
melted_upper <- melt(upper, na.rm=TRUE)

ggplot(data = melted_upper, aes(Var2, Var1, fill = value))+
 geom_tile(color = "white")+
 scale_fill_gradient2(low = "wheat", high = "brown", mid = "white", 
   midpoint = 0, limit = c(-1,1), space = "Lab") +
  theme(
  axis.text.x = element_text(angle = 45, vjust = 1, 
    size = 4, hjust = 1),
  axis.title.x = element_blank(),
  axis.title.y = element_blank(),
  panel.grid.major = element_blank(),
  panel.border = element_blank(),
  panel.background = element_blank(),
  axis.ticks = element_blank())+
  geom_text(aes(Var2, Var1, label = value), color = "gray", size = 2.8) +
  coord_fixed() +
  labs(fill='correlation')  + ggtitle('correlation heatmap')

```


```{r, include=TRUE}
#drop atemp
day1 <- dplyr::select(day1, -c(atemp))
day1
```

```{r, include=TRUE}
# Check Line

fit.all = lm(cnt ~ season + yr + mnth + hr + holiday + workingday + weathersit + temp + hum + windspeed, data = day1)

intercept_only <- lm(cnt ~ 1, data=day1)

forward <- step(intercept_only, direction='forward', 
                scope=formula(fit.all))
summary(forward)

#forward

```

```{r,include=TRUE}
backward <- step(fit.all, direction='backward')
summary(backward)
```
```{r}

day2 <- day1 %>% dplyr::select(-c(casual, registered))
#day2
day2$cnt <- log(day2$cnt)
#day2
x <- model.matrix(day2$cnt~., day2)[,-1]
y <- day2 %>% dplyr::select(cnt) %>% unlist() %>% as.numeric()

#y
grid <- 10^seq(2, -3, by=-.1)

train <- day2 %>% sample_frac(0.8)
test <- day2 %>% setdiff(train)

x_train <- model.matrix(train$cnt~., train)[,-1]
x_test <- model.matrix(test$cnt~., test)[,-1]
cnt <- day2$cnt
#cnt
y_train <- train %>% dplyr::select(cnt) %>% unlist() %>% as.numeric()
y_test <- test %>% dplyr::select(cnt) %>% unlist() %>% as.numeric()
set.seed(1)

#on the full model
out <- glmnet(x, y, alpha = 1, lambda = grid) 

#cv to choose best lambda
cv.out <- cv.glmnet(x_train, y_train, alpha = 1) 
bestlam <- cv.out$lambda.min 
cat('Best lambda obtained is: ', bestlam)

#lasso with best lambda
lasso <- glmnet(x, y, alpha = 1, lambda = bestlam)
predictions <- predict(lasso, type = "coefficients", s = bestlam)
#coef(lasso, s=bestlam)

#remove intercept
lasso.mod <- glmnet(x,y, alpha =1)
beta <- coef(lasso.mod)
beta <- as.matrix(beta)
dim(beta)
lambda <- lasso.mod$lambda
length(lambda)
lam <- rep(lambda, 11)
length(lam)
beta_t <- t(beta)
beta_vec <- as.vector(beta_t)[-c(1:64)]
length(beta_vec)
v <- rownames(beta)[-1]
length(v)
names <- rep(v, each=64)
length(beta_vec)
length(names)
df <- data.frame(lam, names, beta_vec)
plot <- ggplot(df, aes(x = lam, y = beta_vec, color = names)) +
  geom_line() +
  labs(x = "log(lambda)", y = "Coefficient") +
  theme_bw() +
  scale_x_continuous(trans='log10')

plot + ggtitle('Lasso coefficients vs. lambda')
```
```{r}
#x_test
lasso_pred <- predict(lasso, newx = x_test, s = bestlam)
#y_test

#lasso_pred
mae <- mean(abs(y_test - lasso_pred))
mse <- mean((y_test - lasso_pred)^2)
r_squared <- 1 - (sum((y_test- lasso_pred)^2) / sum((y_test - mean(y_test))^2))
mae
mse
r_squared
```



```{r}
day1$cnt <- log(day1$cnt)
mod_forward <- lm(formula = cnt ~ temp + hr + yr + hum + season + holiday + 
    windspeed + weathersit + workingday, data = day1)
plot(mod_forward, which = c(1,2,3,4))
```
```{r}
mod_backward <- lm(formula = cnt ~ season + yr + hr + holiday + workingday + 
    weathersit + temp + hum + windspeed, data = day1)
plot(mod_backward, which = c(1,2,3,4))
```




```{r, include=TRUE}
# Check the variance 
library(car)
ncvTest(fit.all)
```



```{r, include=TRUE}


set.seed(42)
train_index <- createDataPartition(day1$cnt, p = 0.8, list = FALSE)
train_set <- day1[train_index,]
test_set <- day1[-train_index,]

# Train the multiple linear regression model
model <- lm(formula = cnt ~ season + yr + hr + holiday + workingday + 
    weathersit + temp + hum + windspeed, data = train_set)

# Make predictions on the test set
predictions <- predict(model, newdata = test_set)

# Evaluate the model
mae <- mean(abs(test_set$cnt - predictions))
mse <- mean((test_set$cnt - predictions)^2)
r_squared <- 1 - (sum((test_set$cnt - predictions)^2) / sum((test_set$cnt - mean(test_set$cnt))^2))

cat('Mean Absolute Error:', mae, '\n')
cat('Mean Squared Error:', mse, '\n')
cat('R-squared:', r_squared, '\n')

rmse <- function(actual, predicted) {
  return(sqrt(mean((actual - predicted)^2)))
}
rmse_value <- rmse(test_set$cnt, predictions)
cat('Root Mean Squared Error:', rmse_value, '\n')


```
```{r}
plot(cnt ~ temp + hr + yr + hum + season + holiday + 
    windspeed + weathersit + workingday, data = day1)
```



```{r, include=TRUE}
day2 <- day1[ , -which(names(day1) == "cnt")]
pca <- prcomp(day2,scale=TRUE)
variance <- summary(pca)$importance[2,]
df <- data.frame(Component = 1:length(variance), Variance = variance)
df_top_10 <- df[1:10,]
df_top_10 <- df_top_10[order(-df_top_10$Variance),]
df_top_10

pc <- pca$rotation[, 1: 10]
z <- melt(pc)
colnames(z) <- c("Variable", "PC", "value")
plot <- ggplot(z, aes(x = PC, y = Variable, fill= value)) +
 geom_tile(color = 'white')+
 scale_fill_gradient2(low = 'brown', high = 'wheat', mid = 'ivory',
   midpoint = 0, limit = c(-1,1), space = 'Lab')
plot

pca_data <- as.data.frame(predict(pca))
df2 <- pca_data[, 1:2]
df1 <- subset(day1, select = cnt)
combined_df <- cbind(df1, df2)

train_index <- createDataPartition(combined_df$cnt, p = 0.8, list = FALSE)
train_set <- combined_df[train_index,]
test_set <- combined_df[-train_index,]
# Train the multiple linear regression model
model2 <- lm(cnt ~ ., data = train_set)
summary(model2)
# Make predictions on the test set
predictions <- predict(model2, newdata = test_set)
# Evaluate the model
mae <- mean(abs(test_set$cnt - predictions))
mse <- mean((test_set$cnt - predictions)^2)
r_squared <- 1 - (sum((test_set$cnt - predictions)^2) / sum((test_set$cnt - mean(test_set$cnt))^2))
summary(predictions)
```
```{r}
r_squared
mae
mse

```
```{r}
ggplot(df_top_10, aes(x = factor(Component), y = Variance)) +
  geom_bar(stat = "identity", fill = "wheat") +
  scale_x_discrete(labels = 1:10) +
  theme(panel.background = element_rect(fill = "white")) +
  labs(x = "Principal Component", y = "Proportion of Variance Explained",
       title = "Proportion of Variance Explained by Top 10 Principal Components")+
  theme(legend.position = "none")
```





